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<ep-patent-document id="EP91308335B1" file="EP91308335NWB1.xml" lang="en" country="EP" doc-number="0479439" kind="B1" date-publ="19971210" status="n" dtd-version="ep-patent-document-v1-1">
<SDOBI lang="en"><B000><eptags><B001EP>..BE..DE....FR....IT....NL........................</B001EP><B005EP>J</B005EP><B007EP>DIM360   - Ver 2.7 (14 Oct 1997)
 2100000/1 2100000/2</B007EP></eptags></B000><B100><B110>0479439</B110><B120><B121>EUROPEAN PATENT SPECIFICATION</B121></B120><B130>B1</B130><B140><date>19971210</date></B140><B190>EP</B190></B100><B200><B210>91308335.8</B210><B220><date>19910912</date></B220><B240><B241><date>19930719</date></B241><B242><date>19950630</date></B242></B240><B250>en</B250><B251EP>en</B251EP><B260>en</B260></B200><B300><B310>9021246</B310><B320><date>19900929</date></B320><B330><ctry>GB</ctry></B330></B300><B400><B405><date>19971210</date><bnum>199750</bnum></B405><B430><date>19920408</date><bnum>199215</bnum></B430><B450><date>19971210</date><bnum>199750</bnum></B450><B451EP><date>19970124</date></B451EP></B400><B500><B510><B516>6</B516><B511> 6G 02B  27/00   A</B511><B512> 6G 02B   5/04   B</B512></B510><B540><B541>de</B541><B542>Optischer Anzeigeapparat</B542><B541>en</B541><B542>Optical display apparatus</B542><B541>fr</B541><B542>Appareil d'affichage optique</B542></B540><B560><B561><text>EP-A- 0 202 987</text></B561><B561><text>WO-A-84/02197</text></B561><B561><text>WO-A-89/03059</text></B561><B561><text>WO-A-89/12840</text></B561><B561><text>FR-A- 2 096 407</text></B561><B561><text>FR-A- 2 559 278</text></B561><B561><text>GB-A- 2 006 463</text></B561><B561><text>GB-A- 2 088 079</text></B561><B561><text>GB-A- 2 163 869</text></B561><B561><text>GB-A- 2 198 259</text></B561><B561><text>US-A- 3 732 367</text></B561><B561><text>US-A- 4 729 634</text></B561><B562><text>PATENT ABSTRACTS OF JAPAN, vol. 12, no. 288 (P-741); &amp; JP-A-63 064 003</text></B562><B562><text>PATENT ABSTRACTS OF JAPAN, vol. 5, no. 110 (P-71); &amp; JP-A-56 052 707</text></B562><B562><text>ABSTRACT NEW TECHNOLOGY FROM THE AIR FORCE SYSTEMS COMMAND 1977; M.N. ERNSTOFF : 'Liquid Crystal Diffraction Optics HUD'</text></B562><B562><text>PROCEEDING OF THE S.I.D. (SOCIETY FOR INFORMATION DISPLAY) vol. 19, no. 4, 1978, Los Angeles, US, pp. 169-179; M.N. ERNSTOFF : 'A Head-Up Display For The Future'</text></B562></B560><B590><B598>1</B598></B590></B500><B700><B720><B721><snm>Rogers, Philip John</snm><adr><str>24 Cilgant Eglwys Wen,
Bodelwyddan</str><city>Clwyd,
North Wales</city><ctry>GB</ctry></adr></B721></B720><B730><B731><snm>Pilkington P.E. Limited</snm><iid>00268192</iid><adr><str>Glascoed Road</str><city>St Asaph,
Clwyd,
Wales LL 17 0LL</city><ctry>GB</ctry></adr></B731></B730><B740><B741><snm>MacDougall, Donald Carmichael</snm><sfx>et al</sfx><iid>00033372</iid><adr><str>Cruikshank &amp; Fairweather
19 Royal Exchange Square</str><city>Glasgow G1 3AE, Scotland</city><ctry>GB</ctry></adr></B741></B740></B700><B800><B840><ctry>BE</ctry><ctry>DE</ctry><ctry>FR</ctry><ctry>IT</ctry><ctry>NL</ctry></B840><B880><date>19930224</date><bnum>199308</bnum></B880></B800></SDOBI><!-- EPO <DP n="1"> -->
<description id="desc" lang="en">
<p id="p0001" num="0001">The present invention relates to optical display apparatus particularly, although not exclusively, for use as a Head-Up-Display in a fighter aircraft.</p>
<p id="p0002" num="0002">Head-Up-Display (HUD) optics have been known for many years. The conventional form of a HUD optic is a large lens which magnifies and collimates the display on a small cathode ray tube. This collimated display is then reflected off a partially-reflective combiner situated immediately in front of the pilot. The pilot thus sees information (navigation, engine, weapon etc) superimposed on his line of sight and focussed at infinity. Thus, the pilot can, therefore, assimilate essential information without averting his gaze from the outside world or refocussing his eyes. The latter advantages eliminate the approximately two seconds of 'dead' time that are usually required for averting gaze, focussing on instruments, assimilating information, re-directing gaze to the outside world and refocussing at infinity. This 'dead' time could be extremely dangerous in a fast, low-flying fighter aircraft.</p>
<p id="p0003" num="0003">Conveniently, conventional HUD optics comprise folded collimating lenses of the Petzval form, that is two basic groups of positively powered optics separated by a long air-gap in which the<!-- EPO <DP n="2"> --> folding means (usually a plane mirror) is situated. The folding of the optics enables the mechanical axis of the c.r.t. to be approximately parallel to the over-the-nose sight line of the pilot. The depth or profile depth of a conventional HUD optic is nominally only a little less than the diameter of the HUD exit lens and has not been a problem to date in terms of fit into the aircraft. Modern display technology has, however, enabled large, rugged, flat panel displays to be fitted to aircraft and these require a large area of cockpit facia space. Thus it is now required that HUD optics be substantially reduced in depth in order to provide adequate visibility of these flat panel displays. The requirement for a reasonable instantaneous field of view (IFOV) from the HUD, defined only by simple trigonometry involving the size of the HUD exit lens and its distance from the pilot's eyes, has not been relaxed. There are, therefore, apparently contradictory requirements that the HUD exit lens should be large in diameter (in excess of say 160 mm) but the profile depth of the optic, eg the actual physical depth of the box in which the components (c.r.t., folding mirror and collimating lenses) of the optical module are to be accommodated, should be very much less than the exit lens diameter, say 60% of this diameter. This is clearly difficult if not impossible with a conventional optical design.<br/>
<!-- EPO <DP n="3"> -->GB2163869A describes an optical projector for a HUD in which a prism is used to couple light from a CRT display to an output lens. The light undergoes two internal reflections within the prism, enabling the profile depth of the projector to be reduced somewhat relative to the exit diameter of the output lens. GB2198259A describes a similar arrangement for projecting light from two separate CRT displays. WO89/12840 describes an arrangement for coupling light from a CRT to a HUD combiner which comprises a pair of optical surface arranged at an angle to one another. Light passing through the arrangement undergoes two reflections from one of the surfaces and a further reflection at the other of the surfaces before exiting the arrangement to impinge on the combiner.</p>
<p id="p0004" num="0004">An aim of this invention is to overcome the beforementioned problems by the provision of a head-up display optic which has a profile depth which is substantially and preferably much less than the diameter of the exit lens.</p>
<p id="p0005" num="0005">According to the present invention there is provided optical apparatus for superimposing displayed visual information on an observer's view of a scene or object, the apparatus comprising:
<ul id="ul0001" list-style="none" compact="compact">
<li>a modular optical unit (MOU) incorporating a display source (CRT) providing the displayed visual information, collimating optical means having a plurality of lenses with at least an entrance lens (ENL), an exit lens (EXL), and a prism (PM) situated between the entrance lens and the exit<!-- EPO <DP n="4"> --> lens; and</li>
<li>combining means (CM) for combining the displayed visual information with the view of the scene or object,</li>
</ul>    characterised in that the prism (PM) incorporates a short refracting entrance face (ENF) through which display source (CRT) light enters, and two adjacent longer faces (LF, EXF) one of which is the base (LF) of the prism (PM) and the other forming a refracting exit face (EXF), the prism (PM) being arranged so that light entering the prism from the display source (CRT) undergoes three internal reflections before exiting the prism for transmission to the combing means (CM), two internal reflections of light taking place on the base face (LF) and the third taking place on the refracting exit face (EXF), while light is transmitted from the prism (PM) by way of the refracting exit face (EXF), wherein the modular optical unit (MOU) profile depth (PD) is substantially less than the exit lens (EXL) diameter.<!-- EPO <DP n="5"> --></p>
<p id="p0006" num="0006">Preferably the profile depth is less than 60% of the exit lens diameter and may be 40% of the exit lens diameter.</p>
<p id="p0007" num="0007">The prism preferably incorporates a short refracting entrance face through which display source light enters, and two adjacent longer faces one of which is the base of the prism and the other forms a refracting exit face. Three internal reflections of light<!-- EPO <DP n="6"> --> take place in the prism, two on the base face and one on the refracting exit face while light is transmitted from the prism by way of the refracting exit face.</p>
<p id="p0008" num="0008">Preferably the refracting exit face incorporates a wavelength selective dielectric coating, whereas the base face incorporates a highly reflective coating although a dielectric coating may be employed which is highly reflective over the narrow spectral bandwidth of the display source.</p>
<p id="p0009" num="0009">Preferably the angle opposite the refracting entrance face between the base face and the refracting exit face is between 20° and 22°.</p>
<p id="p0010" num="0010">Preferably the display source comprises a cathode ray tube having a mechanical axis which is tilted at a suitable angle with respect to a given horizontal axis, for example of the aircraft within which the optical apparatus is mounted to avoid infringement of the observer's (pilot's) view of the scene or object. The modular optical unit then includes compensating means for correcting for the effect of the angle at which the mechanical axis of the cathode ray tube is tilted. The compensating means may take the form of a fibre optic wedge forming a face plate for the cathode ray tube. The compensating means may alternatively take the form of wedged optical elements located between the cathode ray tube and the prism means to give non-normal incidence at the prism input face and/or a wedge shaped glass faceplate. The exit lens may also be asymmetrical in form.<!-- EPO <DP n="7"> --></p>
<p id="p0011" num="0011">The compensating means may also alternatively be a cathode ray tube whose faceplate is not orthogonal to its mechanical axis.</p>
<p id="p0012" num="0012">The compensating means may alternatively be a Fresnel lens located between the exit lens and the combining means.</p>
<p id="p0013" num="0013">The combining means is preferably of decentered spherical form but may the planar form.</p>
<p id="p0014" num="0014">The invention will be more readily understood from the following description of exemplary embodiments which should be read in conjunction with the accompanying drawings in which:-
<dl id="dl0001" compact="compact">
<dt>Fig 1</dt><dd>shows a head-up display system in accordance with this invention,</dd>
<dt>Fig 2</dt><dd>shows a portion of a head-up display system in accordance with an alternative form of this invention; and,</dd>
<dt>Fig 3</dt><dd>shows a portion of a head-up display system in accordance with a further alternative form of this invention.</dd>
</dl></p>
<p id="p0015" num="0015">Referring to the drawings it should be understood that corresponding components in the various embodiments shown in the drawings have been designated identically.</p>
<p id="p0016" num="0016">The general objective of this invention is to provide a head-up display HUD optic whose profile depth PD is less than the exit diameter of the optic, at the end of the optic facing the pilot. In particular the profile depth to be achieved is typically less than 60% of the exit lens EXL diameter and would ideally be 40% of the exit lens diameter. Generally the ratio of profile depth to exit lens diameter will be 20% less than a conventional HUD optic employing a single reflection.<!-- EPO <DP n="8"> --></p>
<p id="p0017" num="0017">The means by which this is achieved involves the use of a narrow angle triple-bounce prism PM mounted within the main modular optical unit MOU of the head-up display which comprises, amongst other things, a display source in the form of a c.r.t., and at least an entrance lens ENL and exit lens EXL which collimate the display image at a partially reflective spherical combining means CM (see Fig 1) through which the observer/pilot views the outside scene and the display information which is superimposed on the observer's/pilot's line-of-sight and which is focussed at infinity.</p>
<p id="p0018" num="0018">The prism has a short refracting entrance face ENF through which the display light enters and two adjacent longer faces LF, EXF. Face LF is the base of the prism while the other face is a refracting exit face EXF. Three internal reflections of light take place in the prism, PM, two on face LF, and one on the exit face EXF which is also used for final transmission of light from the prism. The angle θ opposite the entrance face ENF between the two longer faces EXF and LF is preferably of the order of 20° to 22°.</p>
<p id="p0019" num="0019">Selective reflection/transmission at the longer faces LF, EXL of the prism PM are achieved partially by total-internal-reflection and partially by the use of coatings C1 and C2. Coating C1 is a wavelength selective dielectric coating operating over the bandwidth of the display source, whereas coating C2 is preferably a highly reflective metallic coating. In some circumstances, however, it may be appropriate to use a dielectric coating for C2 which is only highly reflective over the narrow spectral bandwidth<!-- EPO <DP n="9"> --> of the display source. This acts to reduce the level of solar radiation entering (and exiting in the case of diffuse solar reflection off the display source) the unit.</p>
<p id="p0020" num="0020">There is a potential problem with using a triple-bounce prism PM within the HUD optic in that the input optical axis OA, which usually basically defines the mechanical axis MAC of the c.r.t.(the axis which passes centrally and longitudinally through the c.r.t.), is required to be tilted at such an angle with respect to the aircraft horizontal line ACH that the c.r.t. would seriously infringe the over-the-nose sight line ONL of the aircraft and thereby obscure part of the observer's/pilots view of the scene or object. Generally, therefore, the mechanical axis of the c.r.t. has always to be optimised to be tilted at a suitable angle with respect to the aircraft horizontal line ACH to prevent such infringement occurring. This has the effect of causing the optical input from the display source to be out of alignment with the other components of the modular optical unit.</p>
<p id="p0021" num="0021">This gives rise to a problem which effectively requires means for compensating or correcting for the effect of the c.r.t. angle to enable satisfactory transmission of the display information through the HUD optic.</p>
<p id="p0022" num="0022">This problem is overcome by use of any one of the following solutions:-
<ul id="ul0002" list-style="none" compact="compact">
<li>(a) (see Fig 3) a fibre-optic wedge FOW which serves as the c.r.t. face plate and is an integral part of the c.r.t..<!-- EPO <DP n="10"> --></li>
<li>(b) (see Fig 2) wedged optical elements WO1, WO2 between the c.r.t. and prism, non-normal incidence at the prism input face, and possibly a wedged c.r.t. glass faceplate WFP (which may be a standard c.r.t. with a glass wedge cemented onto it). The exit lens may also be asymmetrical. Non-normal incidence at the prism entrance face ENF acts as though there was a wedge prism in contact with the prism. This arrangement contributes to the tilting of the mechanical axis.</li>
<li>(c) use of a c.r.t. whose faceplate is not orthogonal to its mechanical axis (not shown), the display output being corrected in these circumstances electronically within the c.r.t.</li>
<li>(d) (see Fig 1) use of a Fresnel FRL lens positioned above the exit lens EXL, i.e. between the exit lens EXL and the combiner CM.</li>
</ul></p>
<p id="p0023" num="0023">The combination of the triple-bounce prism PM together with a dielectric coating on its exit face EXF together with one of the means of correcting c.r.t. angle, can provide a large diameter HUD optic of quite a small profile depth PD. Preferably to keep the HUD exit lens EXL as narrow (thin) as possible the lens employed is a single glass aspheric. A filtered narrow-band c.r.t. phosphor (P43 or P53) is also employed to reduce chromatic effects.</p>
<p id="p0024" num="0024">It is important to note that the dielectric coating C1 may not be required if the HUD optic is truncated to a certain extent.<!-- EPO <DP n="11"> --></p>
<p id="p0025" num="0025">Referring to Fig 1, the modular optical unit MOU employs a standard small c.r.t. and the mechanical axis MAC of the c.r.t. is so angled with respect to the over-the-nose line ONL to ensure that this line is not seriously infringed. As a consequence of this, the display information from the c.r.t., which is reflected within the prism PM and then transmitted therefrom is not transmitted towards the combining means CM at the necessary angle to be reflected to the observer. To overcome this problem a suitable Fresnel lens FRL is employed between the exit lens EXL and the combiner CM as mentioned above.</p>
<p id="p0026" num="0026">In Fig. 1 the chain dotted line designated WSC represents the windscreen clearance.</p>
<p id="p0027" num="0027">Referring now to Fig. 2, which shows a typical arrangement of a modular optical unit MOU employing asymmetrical optical elements WFP, WO1 and WO2, wedged, tilted or decentred to overcome the problem caused by the angle of the mechanical axis of the c.r.t. Such optical elements may naturally be located anywhere in the HUD optical system to obtain the necessary effect. It will further be understood tht such wedged, tilted or decentered components may or may not be powered. By way of example, Figure 1 shows a wedged entrance lens ENL.</p>
<p id="p0028" num="0028">A further typical arrangement of the modular optical unit MOU is shown in Fig 3. In this arrangement, to overcome the problem caused by the angle of the mechanical axis of the c.r.t., a fibre optic wedge FOW is employed which abuts the face of the c.r.t..<!-- EPO <DP n="12"> --></p>
<p id="p0029" num="0029">In the Fig 3 arrangement a side band filter SBF is included on the entrance face ENF of the prism. This is provided for removing the side bands of the narrow band phosphor of the display. Such a filter, although not shown in the arrangements of Fig 1 and Fig 2, may be used in these arrangements if required.</p>
<p id="p0030" num="0030">It should be noted that in the arrangements of Fig 2 and Fig 3, the combining means CM is not shown, however, it should be understood that the combiners will the the general form of that shown in Fig 1. These combiners, while shown as of decentered spherical form may also take a planar form if required.</p>
<p id="p0031" num="0031">While the display source employs a cathode ray tube other forms of display could be employed, for instance a rear-illuminated LCD display or other flat panel display device.</p>
</description><!-- EPO <DP n="13"> -->
<claims id="claims01" lang="en">
<claim id="c-en-01-0001" num="0001">
<claim-text>Optical apparatus for superimposing displayed visual information on an observer's view of a scene or object, the apparatus comprising:
<claim-text>a modular optical unit (MOU) incorporating a display source (CRT) providing the displayed visual information, collimating optical means having a plurality of lenses with at least an entrance lens (ENL), an exit lens (EXL), and a prism (PM) situated between the entrance lens and the exit lens; and</claim-text>
<claim-text>combining means (CM) for combining the displayed visual information with the view of the scene or object,</claim-text>    characterised in that the prism (PM) incorporates a short refracting entrance face (ENF) through which display source (CRT) light enters, and two adjacent longer faces (LF, EXF) one of which is the base (LF) of the prism (PM) and the other forming a refracting exit face (EXF), the prism (PM) being arranged so that light entering the prism from the display source (CRT) undergoes three internal reflections before exiting the prism for transmission to the combing means (CM), two internal reflections of light taking place on the base face (LF) and the third taking place on the refracting exit face (EXF), while light is transmitted from the prism (PM) by way of the refracting exit face (EXF), wherein the modular optical unit (MOU) profile depth (PD) is substantially less than the exit lens (EXL) diameter.</claim-text></claim>
<claim id="c-en-01-0002" num="0002">
<claim-text>Optical apparatus as claimed in claim 1, wherein the profile depth (PD) is less than 60% of the exit lens (EXL) diameter.<!-- EPO <DP n="14"> --></claim-text></claim>
<claim id="c-en-01-0003" num="0003">
<claim-text>Optical apparatus as claimed in claim 1, wherein the profile depth (PD) is less than 40% of the exit lens (EXL) diameter.</claim-text></claim>
<claim id="c-en-01-0004" num="0004">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the refracting exit face (EXF) incorporates a wavelength selective dielectric coating (C1).</claim-text></claim>
<claim id="c-en-01-0005" num="0005">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the base face (LF) incorporates a highly reflective coating (C2).</claim-text></claim>
<claim id="c-en-01-0006" num="0006">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the base face (LF) incorporates a dielectric coating (C2) which is highly reflective over the narrow spectral bandwidth of the display source.</claim-text></claim>
<claim id="c-en-01-0007" num="0007">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the angle (θ) opposite the refracting entrance face (ENF) between the base face (LF) and the refracting exit face (EXF) is between 20° and 22°.</claim-text></claim>
<claim id="c-en-01-0008" num="0008">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the display source comprises a cathode ray tube (CRT) having a mechanical axis (MAC) which is tilted at a suitable angle with respect to a given horizontal axis (ACH) to avoid infringement of the observer's view of the scene or object.</claim-text></claim>
<claim id="c-en-01-0009" num="0009">
<claim-text>Optical apparatus as claimed in claim 8, wherein the modular optical unit (MOU) includes compensating means (FOW, WFP, WO1, WO2) for correcting for the effect of the angle at which the mechanical axis (MAC) of the cathode ray tube (CRT) is titled.</claim-text></claim>
<claim id="c-en-01-0010" num="0010">
<claim-text>Optical apparatus as claimed in claim 9, wherein the<!-- EPO <DP n="15"> --> compensating means (FOW, WFP, WO1, WO2) takes the form of a fibre optic wedge (FOW) forming a face plate for the cathode ray tube (CRT).</claim-text></claim>
<claim id="c-en-01-0011" num="0011">
<claim-text>Optical apparatus as claimed in claim 10, wherein the compensating means (FOW, WFP, WO1, WO2) takes the form of wedged optical elements (WO1, WO2) located between the cathode ray tube (CRT) and the prism (PM) to give non-normal incidence at the prism input face (ENF) and/or a wedge shaped glass faceplate (WFP).</claim-text></claim>
<claim id="c-en-01-0012" num="0012">
<claim-text>Optical apparatus as claimed in claim 9, wherein the compensating means (FOW, WFP, WO1, WO2) comprises a cathode ray tube (CRT) whose faceplate (WFP) is not orthogonal to its mechanical axis (MAC).</claim-text></claim>
<claim id="c-en-01-0013" num="0013">
<claim-text>Optical apparatus as claimed in claim 10, wherein the compensating means (FOW, WFP, WO1, WO2) comprises a Frensel lens (FRL) located between the exit lens (EXL) and the combining means (CM).</claim-text></claim>
<claim id="c-en-01-0014" num="0014">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the combining means (CM) is preferably of decentered spherical form.</claim-text></claim>
<claim id="c-en-01-0015" num="0015">
<claim-text>Optical apparatus as claimed in any one of claims 1 to 13, wherein the combining means (CM) takes a planar form.</claim-text></claim>
<claim id="c-en-01-0016" num="0016">
<claim-text>Optical apparatus as claimed in any one of the preceding claims, wherein the exit lens (EXL) is asymmetrical in form.</claim-text></claim>
</claims><!-- EPO <DP n="16"> -->
<claims id="claims02" lang="de">
<claim id="c-de-01-0001" num="0001">
<claim-text>Optischer Apparat, um eine angezeigte optische Information dem Blickfeld eines Beobachters, das einen Schauplatz oder ein Objekt umfaßt, zu überlagern, wobei der Apparat aufweist:
<claim-text>eine modulare optische Einheit (MOU), mit einer Anzeigequelle (CRT), die die angezeigte optische Information liefert, optischen Kollimationsmitteln, die eine Vielzahl von Linsen haben, mit mindestens einer Eingangslinse (ENL), einer Ausgangslinse (EXL), und einem Prisma (PM), das zwischen der Eingangslinse und der Ausgangslinse gelegen ist; und</claim-text>
<claim-text>Kombinationsmittel (CM), um die angezeigte optische Information mit dem Blickfeld, das einen Schauplatz oder ein Objekt umfaßt, zu kombinieren,</claim-text>    dadurch gekennzeichnet, daß das Prisma (PM) eine kurze, brechende Eingangsfläche (ENF) aufweist, über die das Licht der Anzeigequelle (CRT) einfällt, und zwei angrenzende, längere Flächen (LF, EXF) aufweist, von denen eine die Basis (LF) des Prismas (PM) ist, und die andere eine brechende Ausgangsfläche (EXF) bildet, wobei das Prisma (PM) so angeordnet ist, daß das Licht, das von der Anzeigequelle (CRT) in das Prisma einfällt, drei inneren Reflexionen unterworfen wird, bevor es von dem Prisma nach den Kombinationsmitteln (CM) weitergeleitet wird, wobei zwei innere Reflexionen des Lichts an der Grundfläche (LF) erfolgen, und die dritte Reflexion an der brechenden Ausgangsfläche (EXF) erfolgt, und das Licht von dem Prisma (PM) über die brechende Ausgangsfläche (EXF) weitergeleitet wird, wobei die Profiltiefe (PD) der modularen optischen Einheit (MOU) wesentlich kleiner als der Durchmesser der Ausgangslinse (EXL) ist.</claim-text></claim>
<claim id="c-de-01-0002" num="0002">
<claim-text>Optischer Apparat gemäß Anspruch 1, wobei die Profiltiefe (PD) kleiner als 60% des Durchmessers der Ausgangslinse (EXL) ist.</claim-text></claim>
<claim id="c-de-01-0003" num="0003">
<claim-text>Optischer Apparat gemäß Anspruch 1, wobei die Profiltiefe (PD) kleiner als 40% des Durchmessers der Ausgangslinse (EXL) ist.</claim-text></claim>
<claim id="c-de-01-0004" num="0004">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die brechende Ausgangsfläche (EXF) eine wellenlängen-selektive dielektrische Beschichtung (C1) aufweist.</claim-text></claim>
<claim id="c-de-01-0005" num="0005">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die Basisfläche (LF) eine stark reflektierende Beschichtung (C2) aufweist.<!-- EPO <DP n="17"> --></claim-text></claim>
<claim id="c-de-01-0006" num="0006">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die Basisfläche (LF) eine dielektrische Beschichtung (C2) aufweist, die über die schmale spektrale Bandbreite der Anzeigequelle stark reflektierend ist.</claim-text></claim>
<claim id="c-de-01-0007" num="0007">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei der der brechenden Eingangsfläche (ENF) gegenüberliegende Winkel (θ) zwischen der Basisfläche (LF) und der brechenden Ausgangsfläche (EXF) 20° bis 22° beträgt.</claim-text></claim>
<claim id="c-de-01-0008" num="0008">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die Anzeigequelle eine Kathodenstrahlröhre (CRT) aufweist, die eine mechanische Achse (MAC) hat, die unter einem geeigneten Winkel bezüglich einer vorgegebenen, horizontalen Achse (ACH) geneigt ist, um eine Beeinträchtigung des Blickfeldes des Beobachters, das einen Schauplatz oder ein Objekt umfaßt, zu vermeiden.</claim-text></claim>
<claim id="c-de-01-0009" num="0009">
<claim-text>Optischer Apparat gemäß Anspruch 8, wobei die modulare optische Einheit (MOU) kompensierende Mittel (FOW, WFP, WO1, WO2) umfaßt, um die Wirkung des Winkels, unter dem die mechanische Achse (MAC) der Kathodenstrahlröhre (CRT) geneigt ist, zu korrigieren.</claim-text></claim>
<claim id="c-de-01-0010" num="0010">
<claim-text>Optischer Apparat gemäß Anspruch 9, wobei die kompensierenden Mittel (FOW, WFP, WO1, WO2) die Form eines Faseroptikkeils (FOW) haben, der eine Schirmplatte für die Elektronenstrahlröhre (CRT) bildet.</claim-text></claim>
<claim id="c-de-01-0011" num="0011">
<claim-text>Optischer Apparat gemäß Anspruch 10, wobei die kompensierenden Mittel (FOW, WFP, WO1, WO2) die Form von keilförmigen optischen Elementen (WO1, WO2) haben, die zwischen der Kathodenstrahlröhre (CRT) und dem Prisma (PM) angeordnet sind, um einen nicht-senkrechten Einfall bei der Eingangsfläche (ENF) des Prismas zu erhalten, und/oder die Form einer keilförmigen Glas-Schirmplatte (WFP) haben.</claim-text></claim>
<claim id="c-de-01-0012" num="0012">
<claim-text>Optischer Apparat gemäß Anspruch 9, wobei die kompensierenden Mittel (FOW, WFP, WO1, WO2) eine Kathodenstrahlröhre (CRT) aufweisen, deren Schirmplatte (WFP) nicht orthogonal zu ihrer mechanischen Achse (MAC) ist.</claim-text></claim>
<claim id="c-de-01-0013" num="0013">
<claim-text>Optischer Apparat gemäß Anspruch 10, wobei die kompensierenden Mittel (FOW, WFP, WO1, WO2) eine Fresnellinse (FRL) aufweisen, die zwischen der Ausgangslinse (EXL) und den kombinierenden Mitteln (CM) gelegen ist.</claim-text></claim>
<claim id="c-de-01-0014" num="0014">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die kombinierenden Mittel (CM) vorzugsweise eine dezentrierte sphärische Form haben.<!-- EPO <DP n="18"> --></claim-text></claim>
<claim id="c-de-01-0015" num="0015">
<claim-text>Optischer Apparat gemäß irgendeinem der Ansprüche 1 bis 13, wobei die kombinierenden Mittel (CM) eine planare Form haben.</claim-text></claim>
<claim id="c-de-01-0016" num="0016">
<claim-text>Optischer Apparat gemäß irgendeinem der vorhergehenden Ansprüche, wobei die Ausgangslinse (EXL) eine asymmetrische Form hat.</claim-text></claim>
</claims><!-- EPO <DP n="19"> -->
<claims id="claims03" lang="fr">
<claim id="c-fr-01-0001" num="0001">
<claim-text>Appareil optique pour superposer une information visuelle affichée à la vue d'un observateur d'une scène ou d'un objet, l'appareil comprenant:
<claim-text>une unité optique modulaire (MOU) comprenant une source d'affichage (CRT) fournissant l'information visuelle affichée, un moyen optique de collimation comportant plusieurs lentilles avec au moins une lentille d'entrée (ENL), une lentille de sortie (EXL) et un prisme (PM), situé entre la lentille d'entrée et la lentille de sortie; et</claim-text>
<claim-text>un moyen de combinaison (CM) pour combiner l'information visuelle affichée avec la vue de la scène ou de l'objet,</claim-text>    caractérisé en ce que le prisme (PM) comprend une face d'entrée de réfraction courte (ENF), à travers laquelle entre la lumière de la source d'affichage (CRT), et deux faces adjacentes plus longues (LF, EXF), l'une de celles-ci constituant la base (LF) du prisme (PM) et l'autre constituant une face de sortie de réfraction (EXF), le prisme (PM) étant agencé de sorte que la lumière entrant dans le prisme à partir de la source d'affichage (CRT) est soumise à trois réflexions internes avant de sortir du prisme en vue de la transmission au moyen de combinaison (CM), deux réflexions internes de la lumière ayant lieu sur la face de base (LF) et la troisième ayant lieu sur la face de sortie de réfraction (EXF), la lumière étant transmise du prisme (PM) par l'intermédiaire de la face de sortie de réfraction (EXF), la profondeur du profil (PD) de l'unité optique modulaire (MOU) étant substantiellement inférieure au diamètre de la lentille de sortie (EXL).</claim-text></claim>
<claim id="c-fr-01-0002" num="0002">
<claim-text>Appareil optique selon la revendication 1, dans lequel la profondeur du profil (PD) est inférieure de 60% au diamètre de la lentille de sortie (EXL).</claim-text></claim>
<claim id="c-fr-01-0003" num="0003">
<claim-text>Appareil optique selon la revendication 1, dans lequel la profondeur du profil (PD) est inférieure de 40% au diamètre de la lentille de sortie (EXL).</claim-text></claim>
<claim id="c-fr-01-0004" num="0004">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel la face de sortie de réfraction (EXF) comprend un revêtement diélectrique à sélection de la longueur d'onde (C1).<!-- EPO <DP n="20"> --></claim-text></claim>
<claim id="c-fr-01-0005" num="0005">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel la face de base (LF) comprend un revêtement hautement réflecteur (C2).</claim-text></claim>
<claim id="c-fr-01-0006" num="0006">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel la face de base (LF) comprend un revêtement diélectrique (C2) hautement réflecteur au-delà de la largeur de bande spectrale étroite de la source d'affichage.</claim-text></claim>
<claim id="c-fr-01-0007" num="0007">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel l'angle (θ) opposé à la face d'entrée de réfraction (ENF), entre la face de base (LF) et la face de sortie de réfraction (EXF) est compris entre 20° et 22°.</claim-text></claim>
<claim id="c-fr-01-0008" num="0008">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel la source d'affichage comprend un tube à rayons cathodiques (CRT) comportant un axe mécanique (MAC) incliné à un angle approprié par rapport à un axe horizontal défini (ACH) pour empêcher de gêner la vue de l'observateur de la scène ou de l'objet.</claim-text></claim>
<claim id="c-fr-01-0009" num="0009">
<claim-text>Appareil optique selon la revendication 8, dans lequel l'unité optique modulaire (MOU) englobe un moyen de compensation (FOW, WFP, WO1, WO2) pour corriger l'effet de l'angle auquel est incliné l'axe mécanique (MAC) du tube à rayons cathodiques (CRT).</claim-text></claim>
<claim id="c-fr-01-0010" num="0010">
<claim-text>Appareil optique selon la revendication 9, dans lequel le moyen de compensation (FOW, WFP, WO1, WO2) a la forme d'un coin à fibres optiques (FOW) formant une plaque de face pour le tube à rayons cathodiques (CRT).</claim-text></claim>
<claim id="c-fr-01-0011" num="0011">
<claim-text>Appareil optique selon la revendication 10, dans lequel le moyen de compensation (FOW, WFP, WO1, WO2) a la forme d'éléments optiques en coin (WO1, WO2) agencés entre le tube à rayons cathodiques (CRT) et le prisme (PM) pour entraîner une incidence non perpendiculaire au niveau de la face d'entrée du prisme (ENF) et/ou d'une plaque frontale en verre en forme de coin (WFP).</claim-text></claim>
<claim id="c-fr-01-0012" num="0012">
<claim-text>Appareil optique selon la revendication 9, dans lequel le moyen de compensation (FOW, WFP, WO1, WO2) comprend un tube à rayons cathodiques (CRT) dont la plaque frontale (WFP) n'est pas orthogonale par rapport à son axe mécanique (MAC).</claim-text></claim>
<claim id="c-fr-01-0013" num="0013">
<claim-text>Appareil optique selon la revendication 10, dans lequel le moyen de compensation (FOW, WFP, WO1, WO2) comprend une lentille de Fresnel (FRL) agencée entre la lentille de sortie (EXL) et le moyen de combinaison (CM).<!-- EPO <DP n="21"> --></claim-text></claim>
<claim id="c-fr-01-0014" num="0014">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel le moyen de combinaison (CM) a de préférence une forme sphérique décentrée.</claim-text></claim>
<claim id="c-fr-01-0015" num="0015">
<claim-text>Appareil optique selon l'une quelconque des revendications 1 à 13, dans lequel le moyen de combinaison (CM) a une forme plane.</claim-text></claim>
<claim id="c-fr-01-0016" num="0016">
<claim-text>Appareil optique selon l'une quelconque des revendications précédentes, dans lequel la lentille de sortie (EXL) a une forme asymétrique.</claim-text></claim>
</claims><!-- EPO <DP n="22"> -->
<drawings id="draw" lang="en">
<figure id="f0001" num=""><img id="if0001" file="imgf0001.tif" wi="155" he="263" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="23"> -->
<figure id="f0002" num=""><img id="if0002" file="imgf0002.tif" wi="151" he="206" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="24"> -->
<figure id="f0003" num=""><img id="if0003" file="imgf0003.tif" wi="124" he="197" img-content="drawing" img-format="tif"/></figure>
</drawings>
</ep-patent-document>
